{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:54I4N2MSTY2UGFIQNCCTP6HFLH","short_pith_number":"pith:54I4N2MS","schema_version":"1.0","canonical_sha256":"ef11c6e9929e35431510688537f8e559f2fb99a79caab6e45abd39c910b20777","source":{"kind":"arxiv","id":"2208.09949","version":3},"attestation_state":"computed","paper":{"title":"Gravitational Waves-Tomography of Low-Scale-Leptogenesis","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Rome Samanta, Satyabrata Datta","submitted_at":"2022-08-21T19:08:06Z","abstract_excerpt":"A long-lived scalar field ($\\Phi$) which couples weakly to the right-handed (RH) neutrinos ($N_{Ri}$), generates small RH neutrino masses ($M_i$) in Low-Scale-Leptogenesis (LSL) mechanisms, despite having a large vacuum expectation value $v_\\Phi$. In this case, the correlation shared by the $M_i$s and the duration of the non-standard cosmic history driven by the $\\Phi$ provides an excellent opportunity to study LSL signatures on primordial gravitational waves (GWs). We find it engaging, specifically for the gravitational waves that originate due to the inflationary blue-tilted tensor power spe"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2208.09949","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-ph","submitted_at":"2022-08-21T19:08:06Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"ba5e04da3e63ca3061db016638da6bac6b0824a3d96b00d159a860e28845bed3","abstract_canon_sha256":"28d3f5ad8f75ac1d2f614023e88a11ef96c9ac56e926a1ee4eaf6d0565fd1534"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:24:40.820030Z","signature_b64":"KGk0fmGgg/P48ytLwB2clMMH95QBKC5xflxAj3WiBFlJn2v9WRsB9YgFgxlHyb6yYMo7SMcCHA4wt6UX1COMDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef11c6e9929e35431510688537f8e559f2fb99a79caab6e45abd39c910b20777","last_reissued_at":"2026-07-05T05:24:40.819602Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:24:40.819602Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational Waves-Tomography of Low-Scale-Leptogenesis","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Rome Samanta, Satyabrata Datta","submitted_at":"2022-08-21T19:08:06Z","abstract_excerpt":"A long-lived scalar field ($\\Phi$) which couples weakly to the right-handed (RH) neutrinos ($N_{Ri}$), generates small RH neutrino masses ($M_i$) in Low-Scale-Leptogenesis (LSL) mechanisms, despite having a large vacuum expectation value $v_\\Phi$. In this case, the correlation shared by the $M_i$s and the duration of the non-standard cosmic history driven by the $\\Phi$ provides an excellent opportunity to study LSL signatures on primordial gravitational waves (GWs). We find it engaging, specifically for the gravitational waves that originate due to the inflationary blue-tilted tensor power spe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.09949","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2208.09949/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2208.09949","created_at":"2026-07-05T05:24:40.819660+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.09949v3","created_at":"2026-07-05T05:24:40.819660+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.09949","created_at":"2026-07-05T05:24:40.819660+00:00"},{"alias_kind":"pith_short_12","alias_value":"54I4N2MSTY2U","created_at":"2026-07-05T05:24:40.819660+00:00"},{"alias_kind":"pith_short_16","alias_value":"54I4N2MSTY2UGFIQ","created_at":"2026-07-05T05:24:40.819660+00:00"},{"alias_kind":"pith_short_8","alias_value":"54I4N2MS","created_at":"2026-07-05T05:24:40.819660+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.20792","citing_title":"Irreducible Gravitational Wave Background as a Particle Detector","ref_index":94,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH","json":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH.json","graph_json":"https://pith.science/api/pith-number/54I4N2MSTY2UGFIQNCCTP6HFLH/graph.json","events_json":"https://pith.science/api/pith-number/54I4N2MSTY2UGFIQNCCTP6HFLH/events.json","paper":"https://pith.science/paper/54I4N2MS"},"agent_actions":{"view_html":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH","download_json":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH.json","view_paper":"https://pith.science/paper/54I4N2MS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.09949&json=true","fetch_graph":"https://pith.science/api/pith-number/54I4N2MSTY2UGFIQNCCTP6HFLH/graph.json","fetch_events":"https://pith.science/api/pith-number/54I4N2MSTY2UGFIQNCCTP6HFLH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH/action/storage_attestation","attest_author":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH/action/author_attestation","sign_citation":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH/action/citation_signature","submit_replication":"https://pith.science/pith/54I4N2MSTY2UGFIQNCCTP6HFLH/action/replication_record"}},"created_at":"2026-07-05T05:24:40.819660+00:00","updated_at":"2026-07-05T05:24:40.819660+00:00"}